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Metal foams physics PDF

232 Pages·2008·48.939 MB·English
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F O O R P for Viktor and Walter D E T C E R R O C N U F O O R P D E T C E R R O C N U F Preface O A person with a new idea is a crank until the idea sucOceeds. Mark Twain Metal foams show outstanding properties: Low weight, higRh rigidity, high energy absorption capacity, high damping capacity, etc. They have attracted strong in- dustrial and scientific interest during the last decade. A variety of methods has P been developed to produce foams and the development of new, more sophisticated methods is still going on. On the one hand, there are only very few applic ations where metal foams can be directly employed without further processing.DOn the other hand, established metal foam production methods have one feature in common, they produce foam and not metal parts containing metal foam. In the majority of cases additional E shapingandjoiningstepsarenecessarytotransformthemetalfoamintoaworking functional element. In addition, the cellular structure demands for appropriate joining technologies which are often not yeTt available or expensive. As a result, the whole processing sequence is in general long and expensive. The logical consequence of the requCirement to develop cost-effective techniques to produce metal parts with integrated cellular structure is the newly developed process of integral foam molding. Integral foam consists of a solid skin and a cel- lular core. This is the fundamenEtal construction principle which is ubiquitous in biologicalsystems,e.g.thehumanskull,aswellasintechnicalsolutions,e.g.sand- wichconstructions. Theconcentrationofthematerialwithintheskinoptimizesthe R moment of inertia and thus stiffness and strength. Thedevelopmentofmetalbasedintegralfoamfollowsanalogouspathsasthatof polymerswhereintegralfoRamwascommerciallyintroducedinthelate1960s. Poly- mer integral foam parts are now accepted as a material system with characteristic propertieswhichsimplifiesdesigns,reducesproductioncostsandweight,andwhich O increasesstiffnessandoverallstrength. Startingfromlow-pressureinjectionofpoly- mers with small amounts of gas content, highly sophisticated processes have been developedwhereinjectiontakesplaceatveryhighpressuresintomoldcavitieswith C moving elements. Metal integral foams represent – analogous to polymers – an own class of struc- tureswithspNecificpropertiessuchashighstructuralrigidity,highenergyabsorption capacityorhighdamping. Theyarenotthoughttosubstitutestandarddiecastings U VII Preface but open new applications and also demand a specific component design. Com- pared to polymers, the development of metal integral foam molding is just at the beginning. The time delay of four decades between commercialization oFf polymer integralfoammoldingandthecurrentonsetofinvestigationswithrespecttometals canhardlybeexplained. Althoughwehavemadeenormousprogressduringthelast O years of metal integral foam molding research there are still many challenges left which have to be solved in the future to get integral foam components made from light metals into broad industrial application. Nevertheless, weOpresume a large economical potential for metal integral foam molding technologies in the future. Surprisingly, integral foam molding of metals shows much more similarities than differences to polymer integral foam molding. This is not onRly true for the applied molding technologies but also for the resultant integral foam structures and their properties. The intention of this book is to introduce the technological principles P of metal integral foam molding. In addition, its purpose is to reveal the underly- ing physical mechanisms which govern the foam evolution process and which are essential in view of a successful process development . Usually, a first step to gain a physical picture oDf the integral foam molding pro- cess would be to observe it. Unfortunately, in situ experimental observations are impossible since the foaming process takes place in a permanent steel mold within a fraction of a second. Thus, information of tEhe foam formation process has to be extracted from ex situ investigations. This limited information does not help very muchtounderstandtheunderlyingphysicTs. Nevertheless,incombinationwiththe- oreticalinvestigationsandnumericalsimulationtheexperimentalfindingsrevealthe underlying physical principles. C The book is organized in three parts: • Part I: Technology E PartIdescribesthetechnologicalfoundationofintegralfoammoldingofmet- als,atechnologythathasbeenconceivedanddevelopedinourresearchgroup R at the University of Erlangen throughout the last 6 years. For the first time itisshownthatfoamingofmetalsispossiblebyapplyingmoldingtechniques very similar to polyRmer integral foam molding. A low pressure and a high pressure integral foam molding process are introduced and discussed. The moldedpartsshowcompactskinsandfoamedcoreswithporositiesupto80%. O Thermodynamicsandkineticsoftheblowingagentaswellasthelowviscosity of metal melts turn out to be the key for the success of the molding process. Although non-conditioned metal melts are employed, which are generally be- C lieved to be not foamable, the resulting structures are in fact foams. Integral foam molding appears to be the only known process where non-conditioned metal mNelts may be used to produce foam. An explanation of this finding is givenonthebasisofthetheoreticalbackgroundpresentedinPartIIandPart U VIII Preface III. The fact that standard casting alloys may be applied has enormous ad- vantages with respect to casting behavior, properties, recycling and, last but not least, costs. F • Part II: Physics O Thispartisdevotedtothephysicsoffoamingwithspecialemphasisonthevery short time scale which is characteristic for integral foam molding. Although very complex in detail, foam formation is shown to underlieOsimple evolution lawsdeterminedbythewayhowfoamstabilizationisrealized. Basisforthese investigations is a numerical approach which is described in Part III. In or- der to account for the specific situation during integraRl foam molding, foam evolution in the presence of solid particles is discussed in detail. The results of these theoretical considerations represent the basis for the interpretation P of the experimental observations described in Part I. However, the evolution laws are generally valid and can as well be applied to other foam evolution processes. D • Part III: Numerical Simulation The high degree of complexity of foam evolution processes strongly restricts analyticaldescriptions. EvenwiththeaidEofnumericaltools,thesimulationof foamformationprocessesisachallengeduetothehugeandstronglyevolving gas–liquid interface. A new lattice Boltzmann approach for the treatment of T free surfaces is developed and applied on foam evolution problems. For the firsttime,thenumericalsimulationoffoamevolutionstartingfromnucleation C until decay is accessible. The interplay between hydrodynamics, capillary forces, gravity and bubble coalescence processes leads to complex phenomena suchastopologicalrearrangeEments,avalanches,drainage,etc. withoutfurther model assumptions. R Even if integral foam molding of light metals will never find general industrial application,wehavegainedfundamentalinsightsintothemainmechanismsoffoam evolution, especially into tRhe general principles of metal foam stabilization. O Acknowledgments Thisworkisbasedonresultsobtainedduringmyworkastheleaderofthelightweight materialsgroupattheInstituteofScienceandTechnologyofMetalsattheUniver- C sity of Erlangen-Nuremberg. IappreciatethesupportandfreedomIobtainedfromProf. R.F.Singer,thehead of the InstituNte of Science and Technology of Metals, as it enabled me to follow-up and realize own ideas. U IX Preface IwouldliketothankallmembersoftheInstituteforMaterialsSciencewhocon- tributedtothisworkinoneoranotherway. Althoughitisimpossibletoacknowledge all contributors, the work of the following colleagues is especially apprecFiated: M. Arnold, Dr. M. Hirschmann, Dr. M. Thies, A. Trepper and H. Wiehler. In addition, I would like to thank Prof. Rüde, Prof. Kaptay, Prof. Greil and O Prof. Clyne for the support during the habilitation process and the colleagues of Neue Materialien Fürth GmbH for the assistance with the thixomolder. O Carolin Körner, April 2008 R P D E T C E R R O C N U X F Contents O O Preface VII R I TECHNOLOGY 1 1 Introduction P 5 1.1 Integral Foam . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 5 1.2 Polymer Integral Foam Molding . . . . . . . . . . . . . . . . . . . . . 13 D 2 Integral Foam Molding of Metals 19 2.1 Basic Considerations . . . . . . . . . . . . . . . . . . . . . . . . . . . 20 2.2 Admixing of the Blowing Agent . . .E. . . . . . . . . . . . . . . . . . 24 2.3 Low Pressure Integral Foam Molding . . . . . . . . . . . . . . . . . . 27 2.4 High Pressure Integral Foam Molding . . . . . . . . . . . . . . . . . . 32 T 2.5 Base Materials . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 35 2.6 Synopsis . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 41 C 3 Structure and Properties 45 3.1 Density Profiles . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 45 E 3.2 Foam Structure Evolution . . . . . . . . . . . . . . . . . . . . . . . . 55 3.3 Mechanical Properties . . . . . . . . . . . . . . . . . . . . . . . . . . 64 3.4 Synopsis . . . . . . .R. . . . . . . . . . . . . . . . . . . . . . . . . . . 71 II PHYSICS R 73 4 Physics of Foaming 77 O 4.1 Governing Equations . . . . . . . . . . . . . . . . . . . . . . . . . . . 78 4.2 Bubble Dynamics . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 83 4.3 Stabilization Mechanisms. . . . . . . . . . . . . . . . . . . . . . . . . 89 C 5 Evolution Laws 103 5.1 FunNdamentals . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 104 5.2 Non-stabilized Evolution . . . . . . . . . . . . . . . . . . . . . . . . . 106 U XI Contents 5.3 Stabilized Evolution . . . . . . . . . . . . . . . . . . . . . . . . . . . 114 5.4 Synopsis . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 121 F 6 Endogenous Stabilization 123 6.1 Disjoining Pressure . . . . . . . . . . . . . . . . . . . . . . . . . . . . 124 O 6.2 Stratification . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 130 6.3 Foam Evolution . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 131 6.4 Synopsis . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 136 O III NUMERICAL SIMULATION 139 R 7 Theoretical Approach 143 7.1 State-of-the-Art . . . . . . . . . . . . . . . . .P. . . . . . . . . . . . . 144 7.2 Physical Model . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 148 7.3 Lattice Boltzmann Approach. . . . . . . . . . . . . . . . . . . . . . . 152 D 8 LBM for Free Surface Flow 163 8.1 Free Surface and Fluid Advection . . . . . . . . . . . . . . . . . . . . 164 8.2 Interface Boundary Conditions. . . . . . . . . . . . . . . . . . . . . . 167 E 9 LBM for Foam Evolution 171 9.1 Gas Bubbles and Gas Transport T. . . . . . . . . . . . . . . . . . . . . 171 9.2 Interfacial Forces . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 175 9.3 Foam Formation PhenomenaC. . . . . . . . . . . . . . . . . . . . . . . 177 A Gas Supply and Gas Diffusion 185 A.1 Generalized Johnson-MehEl-Avrami Approach . . . . . . . . . . . . . . 185 A.2 Gas Diffusion . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 187 B Miscellany R 189 B.1 Foaming Pressure . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 189 B.2 Mean Cell Diameter . . . . . . . . . . . . . . . . . . . . . . . . . . . 191 R B.3 Curvature Calculation . . . . . . . . . . . . . . . . . . . . . . . . . . 193 C Material ParameOters 195 Symbols 199 C Bibliography 203 Index 221 N U XII F Part I O TECHNOLOGY O R P D E T C E R R O C N U 1 F O O R P D E T C E R R O C N U

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